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According to the measured electron field emission characteristics shown in Figure 7a, planar and patterned CNT-SiNW heterojunctions enable a turn-on electric field of 1.73 and 0.9 V/μm, respectively, while their emission current densities could reach 1.7 and 5.86 mA/cm2, respectively.
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The instrument merges capabilities of measuring the electron field emission current from an individual emitting site and genuine projection of electrons onto a luminescent screen.
ELS is a top hat instrument that measures electrons, and has a 4° × 360° field of view, which is divided into 16 azimuthal sectors, each 22.5° wide.
The film thicknesses and column shapes and sizes were measured by field emission electron microscope (FESEM) (Hitachi S-4100 SEM, Japan).
First, just like the electron is an excitation in the electron field, the Higgs boson is simply a particle which is an excitation of the everywhere-permeating Higgs field.
For the 3D SIB technique they used 2 tangential photon fields and one perpendicular electron field.
The high-resolution images of the Cu patterns were captured and measured using field emission scanning electron microscopy (FESEM, Hitachi S-4800, Jandn) and transmission electron microscopy (TEM, JEM-2010, JEOL, Japan).
The morphology and size of nanoparticles were measured by field emission scanning electron microscope (FESEM-HITACHI SU6600).
The morphologies and size of the ZnO/In2O3 composites were measured by field emission scanning electron microscopy (FESEM; JSM-6700F, Japan).
Film porosity was measured in field emission scanning electron microscopy images.
The diameter and length distribution of the SWCNT measured by field emission scanning electron microscopy which were 0.8 to 1.2 nm and 0.1 to 1 μm, respectively.
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